Consider a system made up of \(N\) particles. The average energy per particle is
given by \(\langle E\rangle=\left(\sum E_{i} e^{-E_{i} / k_{B} T}\right) / Z\)
where \(Z\) is the partition function defined in equation \(36.29 .\) If this is a
two-state system with \(E_{1}=0\) and \(E_{2}=E\) and \(g_{1}=\) \(g_{2}=1,\)
calculate the heat capacity of the system, defined as \(N(d\langle E\rangle / d
T)\) and approximate its behavior at very high and very low temperatures (that
is, \(k_{\mathrm{B}} T \gg 1\) and \(k_{\mathrm{B}} T \ll 1\) ).